Danyłec K, Mazur J, Kozak K, Grządziel D
Institute of Nuclear Physics Polish Academy of Sciences, PL-31342, Kraków, Poland.
J Environ Radioact. 2018 Dec;195:109-113. doi: 10.1016/j.jenvrad.2018.10.004. Epub 2018 Oct 15.
Thoron ( Rn) is a natural radioactive gas, tasteless, odourless, colourless, undetectable without proper equipment. This gas is carcinogenic, just like radon ( Rn) but due to the short half-life (55.6s) and a small amount in the environment, its share in the absorbed radiation dose is often neglected. However, in areas rich in thorium (Th), the radiation dose from the thoron can be much larger and quite significant. The problem is to measure the concentration of the thoron due to its short decay time as well as the fact that it is alpha-emitting as radon. An even greater challenge is to determine the emanation coefficient for the thoron. The method used in this experiment was developed by S.D. Kanse based on the work of D.J Greeman and adapted to the equipment used in Laboratory of Radiometric Expertise IFJ PAN. In the technique used to determine the thoron emanation coefficient, a closed loop system is used in which thoron is pushed out by means of a flow system from the sample and measured by a AlphaGuad DF2000 detector that is adapted to determine concentration of this gas. A sample of the material is placed between 2 filters in the geometry of the sandwich. This arrangement ensures that the thickness of the powder sample is significantly less than the length of the thoron diffusion, thus avoiding significant loss of the thoron due to intergranular absorption and facilitates the complete removal of this gas escaping from the powder. Using this technique, it is important to determine the concentration of Ra and the Th, since for the AlphaGuard detector, the ratio between thoron and radon should not exceed 5:1 for proper determination of the thoron concentration. Measurements of Ra and Th activity were carried out using gamma spectroscopy (HPGe detector). It was examined how the type of filter and grain size of sample affects the obtained results.
钍射气(Rn)是一种天然放射性气体,无味、无臭、无色,没有合适的设备就无法检测到。这种气体具有致癌性,与氡(Rn)一样,但由于半衰期短(55.6秒)且在环境中的含量较少,其在吸收辐射剂量中所占的份额常常被忽视。然而,在富含钍(Th)的地区,钍射气产生的辐射剂量可能会大得多且相当可观。问题在于测量钍射气的浓度,这是因为它的衰变时间短,而且与氡一样会发射α粒子。一个更大的挑战是确定钍射气的析出系数。本实验所采用的方法是由S.D. 坎塞在D.J. 格里曼工作的基础上开发的,并根据波兰科学院核物理研究所辐射测量专业实验室所使用的设备进行了调整。在用于确定钍射气析出系数的技术中,使用了一个闭环系统,在该系统中,钍射气通过流动系统从样品中被推出,并由一台适用于确定这种气体浓度的AlphaGuad DF2000探测器进行测量。将材料样品以三明治结构放置在两个过滤器之间。这种布置确保了粉末样品的厚度远小于钍射气扩散的长度,从而避免了由于颗粒间吸收导致钍射气的大量损失,并便于完全去除从粉末中逸出的这种气体。使用这种技术时,确定镭(Ra)和钍(Th)的浓度很重要,因为对于AlphaGuard探测器来说,为了正确测定钍射气的浓度,钍射气与氡的比例不应超过5:1。使用伽马能谱法(HPGe探测器)对镭和钍的活度进行了测量。研究了过滤器类型和样品粒度如何影响所得结果。